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Find the velocity vector v(t) given the position vector r(t) = (((t)/(2))i + ((t)/(2))j) m.

Physics

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Given the position vector:

r⃗(t)=(cos⁡(t2)i^+sin⁡(t2)j^) m\vec{r}(t) = \left(\cos\left(\frac{t}{2}\right)\hat{i} + \sin\left(\frac{t}{2}\right)\hat{j}\right) \, \text{m}

To differentiate this vector, we differentiate each component with respect to tt. This will give us the velocity vector v⃗(t)\vec{v}(t).

  1. Differentiate the i^\hat{i} component.

    Using the chain rule, ddt(cos⁡(kt))=−ksin⁡(kt)\frac{d}{dt}(\cos(kt)) = -k\sin(kt). Here, k=12k = \frac{1}{2}.

    ddt(cos⁡(t2))=−12sin⁡(t2)\frac{d}{dt}\left(\cos\left(\frac{t}{2}\right)\right) = -\frac{1}{2}\sin\left(\frac{t}{2}\right)
  2. Differentiate the j^\hat{j} component.

    Using the chain rule, ddt(sin⁡(kt))=kcos⁡(kt)\frac{d}{dt}(\sin(kt)) = k\cos(kt). Here, k=12k = \frac{1}{2}.

    ddt(sin⁡(t2))=12cos⁡(t2)\frac{d}{dt}\left(\sin\left(\frac{t}{2}\right)\right) = \frac{1}{2}\cos\left(\frac{t}{2}\right)
  3. Combine the differentiated components to form the velocity vector.

    v⃗(t)=dr⃗dt=(−12sin⁡(t2)i^+12cos⁡(t2)j^) m/s\vec{v}(t) = \frac{d\vec{r}}{dt} = \left(-\frac{1}{2}\sin\left(\frac{t}{2}\right)\hat{i} + \frac{1}{2}\cos\left(\frac{t}{2}\right)\hat{j}\right) \, \text{m/s} v⃗(t)=12(−sin⁡(t2)i^+cos⁡(t2)j^) m/s\boxed{\vec{v}(t) = \frac{1}{2}\left(-\sin\left(\frac{t}{2}\right)\hat{i} + \cos\left(\frac{t}{2}\right)\hat{j}\right) \, \text{m/s}}
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